Tutorial Answers - School of Physics - The University of New South ...
Tutorial Answers - School of Physics - The University of New South ...
Tutorial Answers - School of Physics - The University of New South ...
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9. [K 4.1]. Calculate the minimum photon energy necessary to dissociate the deuteron i.e.<br />
γ + d → p + n. Take the deuteron binding energy to be 2.224589 MeV and use a nonrelativistic<br />
approach.<br />
Conserve energy and linear momentum:<br />
p<br />
γ<br />
→ E<br />
= p<br />
γ<br />
p<br />
+ p<br />
= [ m<br />
p<br />
n<br />
&<br />
+ m ] c<br />
n<br />
E<br />
2<br />
γ<br />
+ m<br />
⎪⎧<br />
⋅ ⎨1<br />
−<br />
⎪⎩<br />
d<br />
c<br />
2<br />
= m<br />
2md<br />
m + m<br />
p<br />
p<br />
c<br />
n<br />
2<br />
+ K<br />
p<br />
+ m c<br />
+ K<br />
⎪⎫<br />
−1⎬<br />
= 2.226219MeV<br />
⎪⎭<br />
10. [A&M 14.11]. On the basis <strong>of</strong> tabulated masses, which <strong>of</strong> the isobars, 17 N, 17 O and 17 F, would<br />
you expect to be the most stable ? Atomic masses are:<br />
17<br />
17<br />
17<br />
M ( N)<br />
= 17.008450 u,<br />
M ( O)<br />
= 16.999131u,<br />
M ( F)<br />
= 17.002095 u,<br />
17 O has the lowest mass and therefore the highest binding energy.<br />
11. [K 5.1] Give the expected shell-model spin and parity assignments for the ground states <strong>of</strong> (a)<br />
7 Li; (b) 11 B; (c) 15 C; (d) 17 F; (e) 31 P and (f) 141 Pr. [(a) 3/2 and –1; (b) 3/2 and –1; (c) 5/2 and +1;<br />
(d) 5/2 and +1; (e) 1/2 and +1; (f) 5/2 and +1]. See left-hand side <strong>of</strong> figure 5.6, p123.<br />
n<br />
2<br />
n<br />
( a)<br />
( b)<br />
( c)<br />
( d)<br />
( e)<br />
( f )<br />
Li,<br />
Z = 3, N = 4. p in 1p<br />
7<br />
11<br />
15<br />
31<br />
B,<br />
Z = 5, N = 6. p in 1p<br />
C,<br />
Z = 6, N = 9.<br />
17<br />
F,<br />
Z = 9, N = 8. p in 1d<br />
P,<br />
Z = 15, N = 16. p in 2s<br />
141<br />
n in 1d<br />
3<br />
2<br />
3<br />
2<br />
5<br />
2<br />
5<br />
2<br />
1<br />
2<br />
Pr, Z = 59, N = 82. p in 2d<br />
∴ I = 3/ 2, π = ( −1)<br />
∴ I = 3/ 2, π = ( −1)<br />
∴ I = 5/ 2, π = ( −1)<br />
∴ I = 5/ 2, π = ( −1)<br />
∴ I = 1/ 2, π = ( −1)<br />
5<br />
2<br />
= ( −1)<br />
= ( −1)<br />
= ( −1)<br />
= ( −1)<br />
∴ I = 5/ 2, π = ( −1)<br />
l<br />
l<br />
l<br />
l<br />
l<br />
1<br />
1<br />
2<br />
2<br />
= ( −1)<br />
l<br />
= −1∴<br />
I<br />
= −1∴<br />
I<br />
= + 1∴<br />
I<br />
= + 1∴<br />
I<br />
0<br />
= ( −1)<br />
= + 1∴<br />
I<br />
2<br />
π<br />
π<br />
π<br />
π<br />
=<br />
=<br />
=<br />
π<br />
=<br />
3 −<br />
2<br />
3 −<br />
2<br />
5 +<br />
2<br />
= + 1∴<br />
I<br />
5 +<br />
2<br />
=<br />
1 +<br />
2<br />
π<br />
=<br />
5 +<br />
2<br />
12. [K5.7] Calculate the shell-model quadrupole moment <strong>of</strong> 209 Bi (I = 9/2 – ). (Experimental value =<br />
–0.37 b).<br />
Q<br />
=<br />
Q<br />
sp<br />
2 j −1<br />
= −<br />
2( j + 1)<br />
⎛<br />
9<br />
2 ⋅ −1⎞<br />
2<br />
3 2<br />
= −⎜<br />
⎟<br />
× × 1.2 × 209<br />
11<br />
2<br />
⎝ ⋅ 5<br />
2 ⎠<br />
r<br />
2<br />
2 j −1<br />
3<br />
= − ⋅ R<br />
2( j + 1) 5<br />
2<br />
3<br />
= −22.13<br />
fm<br />
2<br />
2<br />
2 j −1<br />
3<br />
= − ⋅ R<br />
2( j + 1) 5<br />
= −0.22b<br />
13. [K5.2] <strong>The</strong> low-lying energy levels <strong>of</strong> 13 C are: Ground state (1/2–); 3.09 MeV (1/2+); 3.68<br />
MeV (3/2–) and 3.85 MeV (5/2+). Interpret these states according to the shell-model.<br />
13<br />
C , Z = 6, N = 7.<br />
Protons are paired; the energy states <strong>of</strong> 13 C are determined by the unpaired (7 th ) neutron.<br />
2<br />
0<br />
A<br />
2<br />
3